Densification and Depression in Glass Transition Temperature in Polystyrene Thin Films

Ellipsometry and X-ray reflectivity were used to characterize the mass density and the glass transition temperature of supported polystyrene (PS) thin films as a function of their thickness. By measuring the critical wave vector (q c) on the plateau of total external reflection, we evidence that PS...

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Bibliographic Details
Published inLangmuir Vol. 30; no. 39; pp. 11599 - 11608
Main Authors Vignaud, G, S. Chebil, M, Bal, J. K, Delorme, N, Beuvier, T, Grohens, Y, Gibaud, A
Format Journal Article
LanguageEnglish
Published United States American Chemical Society 07.10.2014
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Summary:Ellipsometry and X-ray reflectivity were used to characterize the mass density and the glass transition temperature of supported polystyrene (PS) thin films as a function of their thickness. By measuring the critical wave vector (q c) on the plateau of total external reflection, we evidence that PS films get denser in a confined state when the film thickness is below 50 nm. Refractive indices (n) and electron density profiles measurements confirm this statement. The density of a 6 nm (0.4 gyration radius, R g) thick film is 30% greater than that of a 150 nm (10R g) film. A depression of 25 °C in glass transition temperature (T g) was revealed as the film thickness is reduced. In the context of the free volume theory, this result seems to be in apparent contradiction with the fact that thinner films are denser. However, as the thermal expansion of thinner films is found to be greater than the one of thicker films, the increase in free volume is larger for thin films when temperature is raised. Therefore, the free volume reaches a critical value at a lower T g for thinner films. This critical value corresponds to the onset of large cooperative movements of polymer chains. The link between the densification of ultrathin films and the drop in their T g is thus reconciled. We finally show that at their respective T g(h) all films exhibit a critical mass density of about 1.05 g/cm3 whatever their thickness. The thickness dependent thermal expansion related to the free volume is consequently a key factor to understand the drop in the T g of ultrathin films.
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ISSN:0743-7463
1520-5827
DOI:10.1021/la501639z